Dashpot

A dashpot is a mechanical device, a damper which resists motion via viscous friction. The resulting force is proportional to the velocity, but acts in the opposite direction, slowing the motion and absorbing energy. It is commonly used in conjunction with a spring (which acts to resist displacement). The process and instrumentation diagram (P&ID) symbol for a dashpot is .

Contents

Types

Two common types of dashpots exist - linear and rotary. Linear dashpots are generally specified by stroke (amount of linear displacement) and damping coefficient (force per velocity). Rotary dashpots will have damping coefficients in torque per angular velocity.

A less common type of dashpot is an eddy current damper, which uses a large magnet inside a tube constructed of a non-magnetic but conducting material (such as aluminium or copper). Like a common viscous damper, the eddy current damper produces a resistive force proportional to velocity.[1][2][3][4]

Dashpots frequently use a one-way mechanical bypass to permit fast unrestricted motion in one direction and slow motion using the dashpot in the opposite direction. This permits, for example, a door to be opened quickly without added resistance, but then to close slowly using the dashpot. For hydraulic dashpots this unrestricted motion is accomplished using a one-way check-valve that allows fluid to bypass the dashpot fluid constriction. Non-hydraulic dashpots may use a ratcheting gear to permit free motion in one direction.

Applications

A dashpot is a common component in a door closer to prevent it from slamming shut. A spring applies force to close the door and the dashpot, implemented by requiring fluid to flow through a narrow channel between reservoirs (often with a size adjustable by a screw), slows down the motion of the door.

Consumer electronics often use dashpots where it is undesirable for a media access door or control panel to suddenly pop open when the door latch is released. The dashpot slows the sudden movement down into a steady and gentle movement until the access door has opened all the way under spring tension.

Dashpots are commonly used in dampers and shock absorbers. The hydraulic cylinder in an automobile shock absorber is a dashpot. They are also used on carburettors, where the return of the throttle lever is cushioned right before the throttle fully closes and then is allowed to fully close slowly to reduce emissions of sudden deceleration (compared to deceleration without a dashpot)

Large forces and high speeds can be controlled by dashpots. For example, they are used to arrest the steam catapults on aircraft carrier decks.

Relays can be made to have a long delay by utilizing a piston filled with fluid that is allowed to escape slowly.

Contactors. Some high energy motor starter contactors have used the dashpot. As in the Allen West type which uses a hydraulic piston. The rod of the piston is part of the built in 'over current' function. The current sensing coil and rod act as a solenoid. The rod is the plunger in the over current coil. During over current the plunger moves up and releases the dropout lever cutting power to the motor. During motor start, current in-rush time is short in comparison with dashpot action and so start current cannot pull the plunger as quick. The damping of the current coil plunger prevents the motor start current from unlatching the dropout lever. On three phase units there is one dashpot for each of the three contactors so excess current in either phase with drop all three contactors as the dropout lever encompasses all contactors.

Viscoelasticity

Dashpots are used to form models of materials that exhibit viscoelastic behavior, such as muscle tissue. Maxwell and Kelvin-Voigt models of viscoelasticity use springs and dashpots in series and parallel circuits respectively. Models containing dashpots add a viscous, time dependent, element to the behavior of solids allowing complex behaviors like creep and stress relaxation to be modeled.

References

  1. ^ Mike Plissi. "Update on eddy-current damping experiments" (pdf). Laser Interferometer Gravitational-Wave Observatory (LIGO). http://www.ligo.caltech.edu/docs/G/G030453-00/G030453-00.pdf. Retrieved 2010-05-29. "A magnet moving inside a non-magnetic conductive tube has its motion retarded. Retardation force is proportional to velocity of magnet- viscous damping." 
  2. ^ Sodano; Bae; Inman; Belvin (June 2006). "Improved Concept and Model of Eddy Current Damper" (pdf). Transactions of the American Society of Mechanical Engineers 128: 294–302. http://www.me.mtu.edu/~hsodano/Publications/ASME%20Vibs-Acoustics%202006%20Improved%20ECD%20-%20Journal%20Version.pdf. "This process of the generation and dissipation of eddy current causes the system to function as a viscous damper" 
  3. ^ Starin; Neumeister (19-21 September 2001). "Eddy Current Damping Simulation and Modeling". Proceedings of the 9th European Space Mechanisms and Tribology Symposium: 321–326. Bibcode 2001ESASP.480..321S. ISBN 92-9092-761-5. "One major advantage of ECD's is their linearity" 
  4. ^ Henry A. Sodano (May 5, 2005). "Development of Novel Eddy Current Dampers for the Suppression of Structural Vibrations" (pdf). Virginia Polytechnic Institute and State University. http://scholar.lib.vt.edu/theses/available/etd-05122005-114434/unrestricted/Complete_Disseration.pdf. Retrieved 2010-05-30. "This damping force can be described as a viscous force due to the dependence on the velocity of the conductor." 

External links